Titlebook: Contact Mechanics and Friction; Physical Principles Valentin L. Popov Book 20101st edition Springer-Verlag Berlin Heidelberg 2010 Adhesion

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Pessary

https://doi.org/10.1007/978-3-662-02005-0tact problems, because in the latter, neither the stress distribution, nor the contact area are known to begin with. The classic solutions from Hertz (non-adhesive contact) and Johnson, Kendall, and Roberts (adhesive contact) use the known solutions for “direct problems” as building blocks to the construction of a solution for a contact problem.

Anguish

https://doi.org/10.1007/978-3-662-02007-4bodies. The fracture strength, and therefore the frictional force, should be, according to this viewpoint, approximately proportionally to the “real” contact area. In this chapter, we will investigate the dependence of the contact area, length, and overall configuration on the normal force.

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